# Active galactic nuclei feedback at parsec scale

## TL;DR

This study uses simulations to analyze how AGN radiation and wind feedback influence accretion flows and outflows at parsec scales, revealing that wind feedback significantly alters outflow properties but not luminosity.

## Contribution

It provides new insights into the effects of wind feedback on outflow characteristics and the limitations of radiative feedback alone in explaining observed AGN luminosities.

## Key findings

- Outflows driven by radiation pressure can be produced with super-Eddington luminosities.
- Wind feedback significantly alters outflow density, temperature, velocity, and kinetic power.
- AGN luminosity remains super-Eddington even with wind feedback, indicating other mechanisms are needed to explain sub-Eddington observations.

## Abstract

We perform simulations to study the effects of active galactic nuclei (AGNs) radiation and wind feedback on the properties of slowly rotating accretion flow at parsec scale. We find that when only radiative feedback is considered, outflows can be produced by the radiation pressure due to Thomson scattering. The mass flux of outflow is comparable to that of inflow. Although strong outflow is present, the luminosity of AGN can be easily super-Eddington. When wind feedback is also taken into account, the mass flux of outflow does not change much. Consequently, the luminosity of the central AGN can still be super-Eddington. However, observations show that the luminosity of most AGNs is sub-Eddington. Some other mechanisms are needed to reduce the AGNs luminosity. Although the mass outflow rate does not change much by wind feedback, other properties of outflow (density, temperature, velocity and kinetic power) can be significantly changed by wind feedback. In the presence of wind feedback, the density of outflow becomes significantly lower, temperature of outflow becomes significantly higher, velocity of outflow is increased by one order of magnitude, the kinetic power of outflow is increased by a factor of $40-100$.